M"Calculating Flywheel Force: Understanding the Two Flywheel Problem | CCM

  • Context: Undergrad 
  • Thread starter Thread starter curiouschris
  • Start date Start date
  • Tags Tags
    Flywheel
Click For Summary
SUMMARY

This discussion focuses on calculating the forces acting on the axles of two flywheels, one spinning at 1000 RPM and the other stationary. The key takeaway is that the linear force on the axle remains constant regardless of the point of application of the force, while torque is influenced by the radius of the flywheel. The friction generated by the second flywheel or a rubber block introduces a torque that affects the axle, and the radius of the flywheel plays a crucial role in determining the energy transfer to the axle. The discussion concludes that understanding the relationship between torque, force, and radius is essential for accurate calculations.

PREREQUISITES
  • Understanding of rotational dynamics and torque
  • Familiarity with concepts of friction and force
  • Knowledge of basic physics principles related to energy transfer
  • Ability to apply mathematical formulas for calculating torque and force
NEXT STEPS
  • Research the formula for calculating torque in rotating systems
  • Study the principles of friction and its role in rotational motion
  • Explore the relationship between radius and energy transfer in rotating objects
  • Learn about real-world applications of flywheel dynamics in engineering
USEFUL FOR

Mechanical engineers, physics students, and anyone interested in the dynamics of rotating systems and the calculations involved in torque and force analysis.

curiouschris
Messages
147
Reaction score
0
Hi all

First of all this is not a homework problem.

Say I have a flywheel of an arbitrary weight and diameter it is fixed in position with a vertical axis and spinning at oh I don't know 1000 revs per min.

Now I bring a second flywheel of the same size and weight which is not spinning at all into contact with the first.

Now my question is how do I calculate the force on the axles of either flywheel.

I am not sure this describes what I am looking for so I will use a clock face analogy to try and make it clearer.

You are looking down at the first flywheel (axle coming out of the screen) and it is spinning clockwise. twelve o'clock is at the top of the screen 6 o'clock at the bottom 3 to the right and 9 to the left.

If the second flywheel came into contact with the first flywheel at the first flywheels 3 o'clock position I imagine the axle of the first flywheel would attempt to move towards the 12 o'clock position, exactly opposite the tangent described at the 3 o'clock position.

With what force would the axle attempt to move? or more precisely how would I calculate that force?

Is that clearer or more muddy?

Please note: the only purpose of the second flywheel is to introduce friction, a rubber block would server the purpose equally well, I am only interested on the forces on the axle of the first flywheel. it just seemed easier to describe that way.

CC
 
Physics news on Phys.org
The linear force on the axle of the first flywheel is the same regardless of the point of application of that force. The point of application of the force only affects the torque about the axis. If the rubber block is generating 10 lbs of force eastward, then there is a eastward 10 lbs of force applied to the axle. The torque would be equal to 10 lbs times the radius of the flywheel.
 
Jeff Reid said:
The linear force on the axle of the first flywheel is the same regardless of the point of application of that force. The point of application of the force only affects the torque about the axis. If the rubber block is generating 10 lbs of force eastward, then there is a eastward 10 lbs of force applied to the axle. The torque would be equal to 10 lbs times the radius of the flywheel.

So neglecting the directional easterly pressure applied by the rubber block the only force on the axle is torque (twisting force).

In other words if I configured the rubber block like the pads in a disc brake, where the flywheel was squeezed equally between two rubber blocks. Then the only force that was 'felt' by the axle was the torque applied by the rapidly slowing flywheel.

Is that correct?

Why wouldn't the axle try to move in the opposite direction to the tangent at the point of contact with the blocks?

CC
 
The force exerting the torque would be friction.
 
The force exerting the torque would be friction.
Of course it would.

Perhaps a drawing may help people understand what I am looking for.

The "unknown force" is the force I am looking for a formula to calculate, I assume it would be an acceleration in the direction indicated.

Please take note the "braking force" is only applied at one point on the flywheels surface, as opposed to the whole surface of the flywheel.
 

Attachments

  • flywheel.png
    flywheel.png
    14.7 KB · Views: 619
curiouschris said:
So neglecting the directional easterly pressure applied by the rubber block the only force on the axle is torque (twisting force).
It can't be ignored. You'd need 2 rubber blocks on opposite sides of the flywheel for the linear forces to cancel and end up with just a torque about the axle.

Why wouldn't the axle try to move in the opposite direction to the tangent at the point of contact with the blocks?
Blocks or block? If there are 2 blocks on opposite sides and they generate equal and opposite forces, then there is no net force on the axle, just a torque. Otherwise there is a linear force that can't be neglected.
 
Jeff Reid said:
Blocks or block?
I did state two blocks, configured as in a disc brake like on a car. so yes two blocks, but not on opposite edges but on opposite sides of the flywheel. If you have seen how a car disc brake works then you'll understand.

See the diagram I uploaded in my previous post.
 
The problem is analogous to spinning up the wheels of a toy car, and then placing the car on the tabletop. The car will accelerate forwards for a few moments while the rotational kinetic stored in the spinning wheels transfers to linear kinetic energy of the whole car (approaching an equilibrium velocity where no more energy transfer occurs, but that's not important here).

If you spin up the wheels again, but this time hold the car's wheels in contact with the tabletop instead of letting it accelerate, then we have a situation similar to your flywheel/brakes scenario. It seems to me that the initial force of friction (per wheel) of the wheels grinding against the tabletop must be equal and opposite to the "pulling" force on each axle (the forwards driving force exerted on the car by the spinning wheels). I only have a minute to finish writing, but at a glance it seems that this pulling force must be the same as the pulling force if you were not holding the car with your hand. Perhaps I've just gone round in a circle, but I find the car analogy easier to understand and the calculation shouldn't be difficult.
 
Hi meta, excellent! that analogy works for me.

So then my question would be, does the radius of the tyre (or flywheel) come into play when calculating the force applied to the axle.

My logic says that if I have two tyres of different radius's but each having the same stored kinetic energy each size tyre will rotate a different amount based on its radius, thus the energy transfer to the axle would be different (per rotation) dependent on the radius of the tyre.

Given two tyres both storing the same kinetic energy the smaller tyre would have to rotate more to push the vehicle the same distance as the larger tyre.

I have answered my own question. Yes the radius does come into play.

Given that I could probably work out the formula I was looking for in my original post.CC
 
Last edited:

Similar threads

  • · Replies 8 ·
Replies
8
Views
3K
  • · Replies 9 ·
Replies
9
Views
2K
  • · Replies 60 ·
3
Replies
60
Views
6K
Replies
12
Views
2K
  • · Replies 49 ·
2
Replies
49
Views
5K
  • · Replies 1 ·
Replies
1
Views
6K
  • · Replies 39 ·
2
Replies
39
Views
5K
  • · Replies 18 ·
Replies
18
Views
8K
Replies
1
Views
2K
  • · Replies 3 ·
Replies
3
Views
6K